青藏高原及周边地区波动E-P通量的分布与变化特征

为了研究青藏高原及周边地区波动E-P通量的分布与变化特征,利用1965～2010年NCEP/NCAR月平均再分析资料,计算了三维E-P通量,经过分析,得到如下主要结论：（1）对流层波动E-P通量的活动中心位于青藏高原南部.（2）波动E-P通量有着明显的季节变化.其中夏季的强度最大,且夏季与冬季相比,垂直分量正负值中心位置的分布几乎相反.从夏季到冬季,E-P通量垂直分量的正值中心逐渐向东北方向移动.（3）波动E-P通量的年代际变化也比较显著.从20世纪70年代中期到80年代前期,波动E-P通量变化平缓;80年代中期至90年代中期,变化很大,90年代中期达到最强,后又开始逐渐变缓.     

黄土高原不同气候区裸地水、热特征对比

为了更好地理解陆地表面水、热通量的空间差异,利用2009年和2010年1月黄土高原陆面过程观测试验（LOPEX）的陆面过程资料,对比分析了不同气候区主要地表水、热通量特征。结果表明：半干旱区的定西在近地层气象要素、土壤湿度、动量通量、地表能量及CO2通量等主要陆面特征物理量与半湿润区的平凉、庆阳差异明显;气候背景相接近的平凉、庆阳的主要陆面特征量比较接近。虽然地形、地势、海拔、下垫面影响因子也是影响陆面特征的重要因素,但是气候背景差异愈明显,陆面特征差异也愈大,即一个地区的气候背景是陆面过程特征的主要决定因子,对陆面特征产生综合影响,而地形、地貌只对一个或几个陆面物理量有影响。     

野外近地表风沙流脉动特征分析

基于风沙流实时测量系统对流沙地表的输沙强度以及不同高度风速进行实时测量所获得的数据,分析野外实际风场中的风沙流脉动特征。结果表明:沙粒的存在削弱平均流场,但对风速的高阶统计矩和分布形式影响不大,不同高度、不同来流平均风速条件下,风沙流中风速仍近似符合高斯分布;瞬时输沙强度服从指数分布,滞后风速约1 s,脉动强烈;30 min输沙强度平均值和脉动标准差均随平均风速的增大而呈幂函数增加,但随风速脉动强度的变化呈先增大后减小的趋势。这意味着脉动风速对输沙率具有重要影响,需要在输沙率预测公式中予以考虑。     

Asymmetric response of the South China Sea SST to El Niño and La Niña

The interannual variability of the sea surface temperature (SST) in the South China Sea (SCS) is investigated according to its relationship with El Nio/La Nia (EN/LN) using monthly products from ICOADS. The SCS SST bears two peaks associated with EN/LN and shows the asymmetric features. Coinciding with the mature phase of EN/LN, the first SST warming/cooling peaks in December(0)-February(1) (DJF(1)) and centers in the southern part. The major difference is in the amplitude associated with the strength of EN/LN. However, the SCS SST anomaly shows distinct difference after the mature phase of EN/LN. The EN SST warm-ing develops a mid-summer peak in June-August(1) (JJA(1)) and persists up to September-October(1), with the same amplitude of the first warming peak. Whereas the LN SST cooling peaks in May(1), it decays slowly until the end of the year, with amplitude much weaker. Comparing with SST and atmospheric circulations, the weak response and early termination of the second cooling is due to the failure of the cyclonic wind anomalies to develop in the northwest Pacific during JJA(1).     

腾格里沙漠东南部野外风沙流观测

风沙流是一种沙粒的群体运动,是风沙物理研究的重要内容之一。开展风沙流研究,能够为风沙运动理论与工程实践提供理论支持。由于自然界风的阵性、地表湿度、下垫面属性和风程长度等影响因子的时空变化对风沙流运动的影响,以及长期野外观测的限制,对风沙流的研究目前还不是很完善。本文依据中国科学院风沙科学观测场2005-2009年的长期观测资料,采用赤池信息量准则（Akaike information criterion）,对5种风沙流通量研究常用的拟合模型进行对比分析。结果表明,指数函数模型(q(z)=ae-z/b)是平坦沙地上风沙流的最佳表示方式,该模型拟合系数a值在0～600之间,但主要分布在0～100之间,占64.40%,其次为100～150之间,占18.24%;系数b值在0～0.06之间,主要分布在0.015～0.040之间,占91.21%,其中0.025～0.030占26.37%,其次为0.030～0.035,占24.40%。风沙流中的沙粒平均跃移高度与拟合系数b相同。风沙流在运动过程中,主要在高度20 cm以下传输。风沙流对地表的风蚀和堆积机率几乎是相等的。     

弱动力浅海中的悬沙输运机制:以天津港附近海域为例

根据在天津港附近海域获取的水动力和浊度数据,分析了悬沙输运特征和输运机制,结果表明:天津港附近海域受不规则半日潮控制呈低流态往复流特征,但涨潮流强于落潮流;涨潮期间底部悬沙浓度与垂线平均流速呈显著线性相关,存在显著的再悬浮作用;潮周期内的悬沙输运呈典型的不对称特征,形成向岸的净输运趋势。输运机制分析结果显示:潮泵效应(尤其是潮汐捕捉效应)是天津港附近海域悬沙输运的主要贡献项,其次是拉格朗日平流输运项,前者比后者高一个量级;垂向剪切作用最小。涨落潮期间流速与悬沙浓度的显著不对称是造成潮汐捕捉效应占主导的基本条件。在潮下带这种悬沙输运格局可能和潮间带发生的细颗粒沉积物捕集(堆积)作用有关。     

The seasonal variability of an air-sea heat flux in the northern South China Sea

The seasonal variabilities of a latent-heat flux (LHF), a sensible-heat flux (SHF) and net surface heat flux are examined in the northern South China Sea (NSCS), including their spatial characteristics, using the in situ data collected by ship from 2006 to 2007. The spatial distribution of LHF in the NSCS is mostly controlled by wind in summer and autumn owing to the lower vertical gradient of air humidity, but is influenced by both wind and near-surface air humidity vertical gradient in spring and winter. The largest area-averaged LHF is in autumn, with the value of 197.25 W/m 2 , followed by that in winter; the third and the forth are in summer and spring, respectively. The net heat flux is positive in spring and summer, so the NSCS absorbs heat; and the solar shortwave radiation plays the most important role in the surface heat budget. In autumn and winter, the net heat flux is negative in most of the observation region, so the NSCS loses heat; and the LHF plays the most important role in the surface heat budget. The net heating is mainly a result of the offsetting between heating due to the shortwave radiation and cooling due to the LHF and the upward (outgoing) long wave radiation, since the role of SHF is negligible. The ratio of the magnitudes of the three terms (shortwave radiation to LHF to long-wave radiation) averaged over the entire year is roughly 3:2:1, and the role of SHF is the smallest.     

草鱼不同养殖模式底泥间隙水与上覆水营养盐的分布特征

于2009年6～10月采集草鱼(Ctenopharyngodon idellus)不同养殖模式围隔底泥的样品,对上覆水和间隙水中营养盐形态与含量进行分析,探讨间隙水和上覆水中营养盐浓度间的相关关系。结果表明:草鱼不同养殖模式围隔大部分间隙水中营养盐浓度要高于上覆水,上覆水与间隙水中PO43--P浓度呈极显著的正相关性(P<0.01)。上覆水和间隙水中的NO2--N和NO3--N浓度垂直分布特征随月变化规律较一致。养殖期间,间隙水溶解态无机氮(DIN)中NH4+-N比例最高,占95%以上。间隙水中NH4+-N浓度随深度增加而逐渐升高(0～10cm),而NO2--N和NO3--N浓度则随深度增加而减小(0～4cm)。表层底泥在0→1cm方向PO43--P浓度明显增加,从2～3cm层后多数养殖模式下浓度缓慢下降,而4→10cm方向上浓度会随深度增加而明显下降。总体而言,三元混养组中(GSL2)上覆水中营养盐的浓度一般要低于GSL1组和GSL3组,且养殖期间该组底层水DO浓度要高于GSL1组和GSL3组,初步认为是一种较为优化的草鱼混养模式。     

Thermodynamic effects on particle movement: Wind tunnel simulation results

Sand/dust storms are some of the main hazards in arid and semi-arid zones. These storms also influence global environmental changes. By field observations, empirical statistics, and numerical simulations, pioneer researchers on these natural events have concluded the existence of a positive relationship between thermodynamic effects and sand/dust storms. Thermodynamic effects induce an unsteady stratified atmosphere to influence the process of these storms. However, studies on the relationship of thermodynamic effects with particles (i.e., sand and dust) are limited. In this article, wind tunnel with heating was used to simulate the quantitative relationship between thermodynamic effects and particle movement on different surfaces. Compared with the cold state, the threshold wind velocity of particles is found to be significantly decrease under the hot state. The largest decrease percentage exceedes 9% on fine and coarse sand surfaces. The wind velocity also has a three-power function in the sand transport rate under the hot state with increased sand transport. Thermodynamic effects are stronger on loose surfaces and fine particles, but weaker on compacted surfaces and coarse particles.     

土壤热扩散率及其温度、热通量计算方法的比较研究

本文利用绿洲系统能量与水分循环过程观测试验的2005年6月11日至15日在甘肃金塔绿洲中部观测的土壤温度、湿度和通量资料,在分析了观测期间土壤温度、湿度和通量特征的基础上,采用振幅法、相位法、谐波法和热传导对流法计算了5~20 cm土壤层的土壤热扩散率.在此基础上,以深度为5 cm的土壤层为上边界条件,计算了10 cm、20 cm深度的土壤温度和10 cm深度的热通量.结果表明:谐波法能很好地计算土壤温度,10 cm和20 cm深度的计算值相对观测值的标准差分别为:0.21 ℃和0.18 ℃;热传导对流法计算的土壤温度好于振幅法和相位法,但由于忽略了土壤水分通量密度的日变化,该方法用于土壤含水量有明显日变化的浅层土壤时,会出现计算误差.谐波法的计算土壤热通量与实测值最为接近,计算值与实测值的相关系数达到0.868.